2016
DOI: 10.1002/sia.5933
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Accurate peak fitting and subsequent quantitative composition analysis of the spectrum of Co 2p obtained with Al Kα radiation: I: cobalt spinel

Abstract: Employing state‐of‐the‐art and practical peak‐fitting and background modeling methods (active approach), we obtained high quality fitting of the photoemission spectrum of Co 2p in cobalt spinel. The concurrent analysis of both 2p3/2 and 2p1/2 branches played a fundamental role. It revealed various Auger features that interfere with the main photoemission lines. It was possible to accurately reproduce the corresponding composition (Co3O4.0 ± 0.25) and to report the relative intensity of the various multiplet/sa… Show more

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Cited by 122 publications
(79 citation statements)
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“…The intensity of the satellite features appears to be enhanced indicating a contribution from the presence of Co(OH) 2 and phosphate species on the surface. 52 As shown in Figure 1h, two peaks, P 2p 3/2 and P 2p 1/2 , were also present in the P 2p region at 132.3 and 133.2 eV, respectively. These peaks are consistent with the characteristic binding energies of tetrahedral (PO 4 ) groups.…”
Section: Preparation and Characterization Ofmentioning
confidence: 78%
“…The intensity of the satellite features appears to be enhanced indicating a contribution from the presence of Co(OH) 2 and phosphate species on the surface. 52 As shown in Figure 1h, two peaks, P 2p 3/2 and P 2p 1/2 , were also present in the P 2p region at 132.3 and 133.2 eV, respectively. These peaks are consistent with the characteristic binding energies of tetrahedral (PO 4 ) groups.…”
Section: Preparation and Characterization Ofmentioning
confidence: 78%
“…The spectra quantification was done employing an approach that evaluates the signal attenuation due to inelastic and elastic scattering . The method has been proven successful in the chemical assessment of other first‐row transition metal oxides (Co 3 O 4 and Fe 2 O 3 ) and in many other materials reported by this group and others. The composition of a zinc oxide overlayer was evaluated considering that the atomic density ( ρ S ) of each element ( S = Zn 2 p [metal], Zn 2 p [oxide], O 1 s , C 1 s ) is related to the corresponding peak intensity ( I S ) through the following set of equations: IS()α=C0.12emρS0.12emnormaldσSnormaldΩAS0.12emλSsinα0.5em[]1exp()dSλS0.12emsinα0.5emicentercenterlayerscenteraboveSexp()diλS,normali0.12emsinα, where d σ S /d Ω is the differential photoelectron cross section of core level S , A S is the efficiency of the spectrometer at the associated electron kinetic energy, λ S is the effective attenuation length as the photoelectron travels through the layer containing species S , d S is the thickness of such layer, α is the take‐off angle, λ S , i is the effective attenuation length of the photoelectrons from species S as they travel through layer i in the way out to the surface (so the last factor is the attenuation caused by the material above layer S ), d i is the thickness of layer i , and C is an overall constant (the same for every species) that depends on the X‐ray flux and other geometrical parameters .…”
Section: Resultsmentioning
confidence: 99%
“…As can be seen in Fig. 3(a), the Ni 2p spectra for NiMoSAC was Meanwhile, the Co 2p spectrum was fitted considering a LMM Auger peak at 774.6 eV, 43 cobalt sulfide phases Co x S y like Co 2 S 3 , Co 9 S 8 , or CoS (BE at 778.4 eV), 37,44 a peak at 779.4 eV arising from the CoMoS phase, cobalt oxide (Co OX ) with BE at 782.5 eV, which is close to that of Co in Co 2 O 3 (781.4 eV) or Co(OH) 2 (782 eV) but not with the BE of Co in CoO (780 eV), 12 as shown in Fig. 3(c).…”
Section: B Mo-speciesmentioning
confidence: 99%